System and method for electromechanical activation of arrhythmias

ABSTRACT

Systems and methods for detecting electromechanical wave propagation within a body structure of a patient in a series of image frames representing movement the body structure are provided. Image data is acquired comprising a series of image frames corresponding to the movement of a body structure. A correlation calculation is performed on the image frames to generate a displacement map representing the relative displacement between the first and second image frames. A video is generated comprising a series of displacement maps. The parameters of movement of the body structure are detected by analysis of the displacement maps. The image acquisition can detect the movement of the body structure without inducing such movement.

CROSS REFERENCE TO RELATED APPLICATIONS

This application is a divisional of U.S. patent application Ser. No.15/048,761, entitled “System and Method for Electromechanical Activationof Arrhythmias”, filed Feb. 19, 2016, now allowed, which is acontinuation in part of U.S. patent application Ser. No. 14/449,820,entitled “Systems And Methods For Electromechanical Wave Imaging of BodyStructures”, filed Aug. 1, 2014, which is a continuation of U.S. patentapplication Ser. No. 11/433,510, entitled “Systems And Methods ForElectromechanical Wave Imaging of Body Structures”, filed May 12, 2006,which issued as U.S. Pat. No. 8,858,441 on Oct. 14, 2014, which claimspriority to U.S. Provisional Application No. 60/680,081 entitled“Systems And Methods For Electromechanical Wave Imaging of BodyStructures”, filed on May 12, 2005, each of which is incorporated hereinby reference in its entirety and from each of which priority is claimed.This application also claims priority from U.S. Provisional ApplicationNo. 62/118,402, filed Feb. 19, 2015, which is incorporated by referenceherein in its entirety.

A portion of the disclosure of this patent document contains materialwhich is subject to copyright protection. The copyright owner has noobjection to the facsimile reproduction by anyone of any portion of thepatent document, as it appears in any patent granted from the presentapplication or in the Patent and Trademark Office file or recordsavailable to the public, but otherwise reserves all copyright rightswhatsoever.

STATEMENT REGARDING FEDERALLY-SPONSORED RESEARCH

This invention was made with government support from the NationalInstitutes of Health under Grant Nos. R01EB006042, R21HL096094 andR01HL114358. The government has certain rights in the invention.

BACKGROUND

This present disclosed subject matter relates to techniques for imagingand detecting the propagation of mechanical waves within a bodystructure of a patient.

Certain medical conditions, such as diagnosis of myocardial ischemia,can be difficult to establish in their early stages when treatment ismost effective. Patients suffering from myocardial ischemia can presentto an emergency room or acute care facility with typical cardiacsymptoms such as chest pain, described as tightness, pressure, orsqueezing, but some patients can have other symptoms such as arm or chinpain, nausea, sweating, or abdominal pain. Certain techniques such aselectrocardiogram often provide inconclusive findings regardingischemia, and sometimes can even be unable to identify situations inwhich ischemia has progressed to cell damage and myocardial infarction(MI). Other techniques are available for diagnosing infarction relativeto its predecessor, ischemia. For example, a blood test to measure thecreatine kinase-MB (CK-MB) enzyme level is used for detection ofmyocardial cell damage. Other serum markers include troponin I, and to alesser extent, myoglobin. However, the blood levels of certain suchcompounds can take several hours to rise, so that diagnosis of MI can bedelayed. Reliance on blood tests alone can result in a significant lossof time when early aggressive therapy is warranted.

Certain less invasive diagnostic techniques have become availablethrough the observation of mechanical properties of tissue via imagingtechniques. Such evaluation of the function of the heart, cardiovasculartissue, or other body structures can be based on the mechanicalinterpretation of the movement of the these structures, such as, forexample, the active contractions and passive relaxation of themyocardium.

Using certain imaging techniques, the evaluation of the heart functioncan be based on a single mechanical interpretation of myocardialdeformation. By use of these techniques, the deformations of themyocardium can be quantified over a complete cardiac cycle in order toprovide some information on the myocardial viability.

Certain low frequency mechanical vibrations in the heart are known inhuman patients. Certain ultrasound techniques can be used to obtainpulsive mechanical vibrations around end-systole and end-diastole in thefrequency range of 25 to 100 Hz.

Additionally, atrial arrhythmias are a known and can cause of morbidityand mortality. Certain mechanical factors, such as chamber size and walltension, can affect the onset and perpetuation of atrial arrhythmia.Certain echocardiographic measurements can also be used to characterizeatrial arrhythmias. Yet, systems and techniques to analyze the 2-Dspatio-temporal evolution of the local deformations of the atria duringe.g., focal tachycardia, flutter, and fibrillation, would be beneficial.

Accordingly, there is a need for a noninvasive imaging modality whichprovides insight into the source or focus of an arrhythmia.

SUMMARY

The present disclosure provides elasticity imaging techniques toevaluate mechanical wave propagation, and provide an estimation ofelectrical propagation in a noninvasive manner.

In example embodiments, the disclosed subject matter provides systemsand methods for detecting wave propagation within the tissue of apatient in a series of image frames representing movement of such tissueof the body structure. Image data is acquired comprising a series ofimage frames corresponding to the movement of the tissue. In anexemplary embodiment, the tissue can be the wave propagation in themyocardium. In another exemplary embodiment, the movement of body tissuecan be wave propagation in the arteries or the aorta.

A correlation calculation can be performed on the image frames togenerate a matrix with the location of correlation maxima representingthe relative displacement between the first and second image frames,also referred to as a displacement map. A video can be generatedcomprising a series of displacement maps. The parameters of movement ofthe cardiac structure can be detected, such as velocity, attenuation,frequency, etc. The wave can be a shear wave, representative of theelectrical wave propagation within the body structure.

According to another aspect of the present disclosure, systems andmethods are provided for mapping electromechanical activity during anarrhythmia. Image information of a heart of a subject can be obtainedusing an imaging device. A strain map of the heart can be generated fromthe image information. Occurrences of a first electromechanical event ofthe heart and a second electromechanical event can be determined fromthe strain map. A spatio-temporal map of atrial and ventricularmechanics of the heart can be generated by tracking the onset of thefirst and second event for each pixel of a heart wall of the subjectidentified from the image information. A representative mechanical cycleassociated with a contraction of the heart can be identified using thespatio-temporal map.

For example, electromechanical activation mapping can characterizepropagation patterns of electromechanical strains during focal andreentrant arrhythmias of the heart.

Additionally, regions in which the mechanical and electrical activitiesare decoupled can be identified by mapping the electromechanicalactivity of the heart.

Furthermore, the spatio-temporal map can be generated by obtainingisochrones strongly correlated to electrical isochrones by tracking apropagation front of an end-diastole electromechanical activation of theheart.

In addition, a type of cardiac arrhythmia present in the heart can bedetermined from the information collected in the ultrasound scan of theheart. Upon identifying that the cardiac arrhythmia present in the heartincludes focal rhythms, an onset of ventricular contraction can bedetermined by identifying a first zero-crossing of an incrementalstrains occurring after an onset of a P-wave on an electrocardiogram.Upon determining that the cardiac arrhythmia present in the heart is atype of reentrant arrhythmia, a high-resolution Fourier transform can beperformed using a generalized Goertzel algorithm to interpolate strainsignals in Fourier space for each individual pixel in an atria of theheart.

For example, a peak mechanical cycle length (MCL) map can be generatedby selecting a MCL having a highest amplitude within thephysiologically-relevant time range for each pixel of the ultrasoundscan of the heart, such that the MCL map identifies, for each pixel ofthe atria, which cycle length is most present in a Fourier spectrum ofcycle lengths. The cycle length best representing an atrial contractionof the heart can be determined. A phase corresponding to the determinedcycle length can be determined to map a propagation of a mechanicaloscillation of the heart at the determined cycle length.

Additionally, the ultrasound scan further can be performed by emitting acircular ultrasonic wave to instruct an ultrasound apparatus to performa motion estimation sequence. A B-mode acquisition can be performed tocapture heart anatomy of the heart. A plurality of beams can begenerated to reconstruct frames from the motion estimation sequenceusing a delay-and-sum algorithm with a reconstructed sampling frequency.

BRIEF DESCRIPTION OF THE DRAWINGS

The patent or application file contains at least one drawing executed incolor. Copies of this patent or patent application publication withcolor drawings will be provided by the U.S. Patent and Trademark Officeupon request and payment of the necessary fee.

FIG. 1 is a diagram illustrating the system in accordance with thepresent disclosure.

FIG. 2 is a diagram illustrating exemplary stages in a method inaccordance with the present disclosure.

FIG. 3 is a diagram illustrating a technique for measuring movement ofstructures within an image in accordance with the present disclosure.

FIG. 4 is a chart representing the velocity of structures within animage in accordance with the present disclosure.

FIG. 5 illustrates a technique of detecting wave propagation inaccordance with a further embodiment of the present disclosure.

FIG. 6 illustrates a technique of detecting wave propagation inaccordance with yet another embodiment of the present disclosure.

FIGS. 7(a)-11(b) are images illustrating the propagation of a wavewithin a body structure in accordance with an exemplary embodiment ofthe present disclosure.

FIGS. 12(a)-18(b) are images illustrating the propagation of a wavewithin a body structure in accordance with another exemplary embodimentof the present disclosure.

FIG. 19 is an ultrasound image of a mouse left ventricle in aparasternal long-axis view.

FIG. 20(a) is an axial displacement map overlaid to the grayscale B-modeimage of the left ventricle during systole in accordance with thepresent disclosure.

FIG. 20(b) is an axial displacement map overlaid to the grayscale B-modeimage of the left ventricle during diastole (relaxation phase) inaccordance with the present disclosure.

FIG. 20(c) is an ECG indicating the time of the acquisition during thecardiac cycle of FIG. 20(a) in accordance with the present disclosure.

FIG. 20(d) is an ECG indicating the time of the acquisition during thecardiac cycle of FIG. 20(b) in accordance with the present disclosure.

FIG. 21(a) is a time plot illustrating the temporal variation of theaxial displacements estimated on one central RF-line as line plotted onFIG. 20(b) in accordance with the present disclosure.

FIG. 21(b) illustrates the frequency content of the displacementvariation in the septum at the depth of 12.5 mm plotted as a function oftime in accordance with the present disclosure.

FIG. 21(c) is a time plot illustrating the temporal variation of theaxial displacements after bandpass filtering of the plot illustrated inFIG. 21(a) showing the transient and high frequency components inaccordance with the present disclosure.

FIG. 21(d) illustrates the ECG signal acquired simultaneously with thedata illustrated in FIGS. 21(a)-(c) in accordance with the presentdisclosure.

FIGS. 22(a)-(d) illustrate a sequence of axial displacement mapsoverlaid to the grayscale B-mode image of the left ventricle aroundend-systole taken every 0.6 ms showing the propagation of a firstmechanical wave front in the septum in accordance with the presentdisclosure. The arrows indicate the progression of the wave front in theseptum.

FIGS. 22(e)-(f) illustrate a sequence of axial displacement mapsoverlaid to the grayscale B-mode image of the left ventricle aroundend-systole taken every 0.6 ms showing the propagation of a secondmechanical wave front in the septum in accordance with the presentdisclosure. The arrows indicate the progression of the wave front in theseptum.

FIGS. 22(g)-(l) illustrate the ECG signal plotted below each respectiveimage of FIGS. 22(a)-(f) indicating the time t of the acquisition duringthe cardiac cycle in accordance with the present disclosure.

FIG. 23 is a plot illustrating the distance of propagation as a functionof the phase of the end-systolic wave at three frequencies in accordancewith the present disclosure.

FIGS. 24(a)-(f) illustrate a sequence of axial displacement mapsoverlaid to the grayscale B-mode image of the left ventricle around thebeginning of systole taken every 2.8 ms, showing the propagation of astrong mechanical wave in the posterior wall in accordance with thepresent disclosure. The arrows indicate the progression of the wavefront in the posterior wall.

FIGS. 24(g)-(l) illustrate the ECG signal plotted below each respectiveimage of FIGS. 24(a)-(f) indicating the time t of the acquisition duringthe cardiac cycle in accordance with the present disclosure.

FIG. 25 is a plot illustrating the distance of propagation as a functionof the phase of the wave at the frequency of 80 Hz during the beginningof systole transient motion in accordance with the present disclosure.

FIGS. 26(a)-(e) illustrate a sequence of axial displacement mapsoverlaid to the grayscale image (0.12 ms between successive frames)indicating an electromechanical wave propagating in the posterior wallof the mouse from the apex towards the base during pacing in the rightatrium close to the sinoatrial node in accordance with the presentdisclosure.

FIGS. 26(f)-(j) illustrate the ECG signal plotted below each respectiveimage of FIGS. 26(a)-(e) indicating the time t of the acquisition duringthe cardiac cycle in accordance with the present disclosure.

FIGS. 27(a)-(e) illustrate a sequence of axial displacement mapsoverlaid to the grayscale image (0.07 ms between successive frames)indicating an electromechanical wave propagating in the posterior wallof the mouse from the base towards the apex during pacing in the rightventricle close to the base in accordance with the present disclosure.

FIGS. 27(f)-(j) illustrate the ECG signal plotted below each respectiveimage of FIGS. 27(a)-(e) indicating the time t of the acquisition duringthe cardiac cycle in accordance with the present disclosure.

FIGS. 28(a)-(f) illustrate a sequence of axial displacement mapsoverlaid to the grayscale B-mode image of the aorta taken every 0.7 ms.Sequence of images showing the propagation of the pulse wave in theaorta. The arrows indicate the progression of the wave front in theaorta

FIGS. 28(g)-(l) illustrate the ECG signal plotted below each respectiveimage of FIGS. 26(a)-(f) indicating the time t of the acquisition duringthe cardiac cycle in accordance with the present disclosure.

FIG. 29 illustrates the distance of propagation as a function of thephase of pulse wave at the frequency of 80 Hz. The slope of the curvegives the pulse wave velocity in accordance with the present disclosure.

FIGS. 30(a)-(c) illustrates examples of high temporal resolution strainsduring different types of arrhythmia in accordance with the presentdisclosure.

FIGS. 31(a)-(d) illustrates examples of propagating electromechanicalactivation in atria of normal subjects and a patient undergoing focalatrial tachycardia in accordance with the present disclosure.

FIGS. 32(a)-(d) illustrates analysis of reentrant arrhythmias using asingle-frequency atrial flutter case using a peak cycle length map,cycle length histogram, a phase map, and electrogram in accordance withthe present disclosure.

FIG. 33(a) illustrates peak cycle length maps in two atrial flutterpatients in accordance with the present disclosure. FIG. 33(b)illustrates a correlation between mechanical cycle length (MCL) andelectrical cycle length in five atrial flutter patients in accordancewith the present disclosure. FIG. 33(c) illustrates a peak cycle lengthmap during atrial fibrillation in accordance with the presentdisclosure. FIG. 33(d) illustrates a histogram depicting spatialfragmentation of peak cycle length during atrial fibrillation inaccordance with the present disclosure.

Throughout the figures, the same reference numerals and characters,unless otherwise stated, are used to denote like features, elements,components or portions of the illustrated embodiments. Moreover, whilethe present disclosure will now be described in detail with reference tothe figures, it is done so in connection with the illustrativeembodiments.

DETAILED DESCRIPTION

The system and methods described herein can be useful for analyzing dataobtained by an image generating device, such as an ultrasoundtransducer. The systems and methods can also be useful for measuringmechanical properties and estimating the electrical characteristics of abody tissue structure or organ, such as, for example, the myocardium orthe aorta.

For example, the disclosed subject matter can be used in connection withimaging and characterizing the propagation of electromechanical waves inthe heart. During the cardiac cycle, electrical waves propagate in themyocardium in order to induce its contraction. Contraction of themyocardial fibers results in a strong mechanical wave, which, since itresults from the coupling of the electrical excitation and themechanical properties of the myocardium, is referred to herein as an“electromechanical wave.” The speed of this wave is a function of theelectrical and mechanical properties of the myocardium, and, accordingto the present disclosure, can be used to detect changes in theseproperties to diagnose heart diseases.

An exemplary embodiment of the system is illustrated in FIG. 1 anddesignated system 100. System 100 can include an image detection device,such as ultrasound probe 102, which is used to create images of theheart H or other organ or structure of the patient P. The imagedetection device does not induce discernible vibration in the bodystructure, and merely detects pre-existing motion. The signals detectedby the probe 102 can be transferred to an ultrasound scanner 104. Theexemplary embodiments described herein are designed to work withconventional ultrasound scanners. For example, commercial portablescanners, such as Terason 2000, high frequency scanners, such asVisualsonics Vevo 770, and routinely used clinical scanners, such as GESystem Five or GE Vivid Five or Seven, are useful for image acquisitionin accordance with the exemplary embodiments. The raw data produced bythe scanner 104 can be transferred to a computer 106 having a CPU 108for processing the data. In the exemplary embodiment, the computer andCPU would be Dell PC with a 2 GHz processor. It is understood that thecomputer and CPU can also be integrated with the ultrasound scanner 104.Also useful in the system would be storage such as disk drives, forstoring data on input files 110 and for writing output onto output files112. As will be described herein, input files 110 can includeinformation such as thresholds. Output files 112 can include thedisplacement maps, videos of myocardium displacements, or computed data,such as electromechanical wave properties. It is understood that apreprogrammed chip can be used to execute the algorithms describedherein. Typically, an output device, such as monitor 114, and an inputdevice, such as keyboard 116, are also components of the system.

In accordance with an exemplary embodiment, the methods described hereinare particularly useful for imaging the propagation of electromechanicalwaves in the heart. A method for detecting the properties of theelectromechanical wave are described herein and represented in FIG. 2.In an early stage in the procedure, raw imaging data of the bodystructure is acquired by image acquisition equipment such as theultrasound probe 102 and scanner 104. In the exemplary embodiment, a setof N frames of raw ultrasound data of the heart is acquired during acardiac cycle at high frame rate, e.g., higher than 100 fps, althoughframe rates of about 56 fps and 170 fps, etc., yield useful results(202). The selected frame rate should be commensurate with the speed ofthe propagation of the movement, such as the wave, being studied. Theelectrocardiogram (EKG) can also be recorded. The raw data can bedigitized and stored in real-time in the scanner memory.

In a subsequent stage, the data can be transferred to a computer forprocessing (204). In an exemplary embodiment, the transfer can occurusing a protocol such as Ethernet TCP IP. This is optional, as thecomputer can be integrated with the scanner 104.

At 206, the raw data received from the image acquisition equipment isprocessed. In the exemplary embodiment, the data processing computes anestimation of the displacement of particular objects in the images, suchas the myocardium, between consecutive frames. Typically this processingoccurs off-line; however, it is understood that this procedure can occursequentially subsequent to receiving two consecutive frames. Accordingto the exemplary embodiment, axial displacements (in the direction ofthe transducer) are computed. Lateral, or elevational, displacements(perpendicular to the transducer) can also be computed using a similartechnique, for example, as disclosed in Konofagou E. E. and Ophir, J.,(1998), A New Elastographic Method for Estimation and Imaging of LateralStrains, Corrected Axial Strains and Poison's Ratios in Tissues,”Ultrasound in Medicine and Biology 24(8), 1183-1199 (1998); Konofagou etal. (1998), Three-dimensional Motion estimation in Elastography, IEEEProceedings of the Symposium of Ultrasonics, Ferroelectrics andFrequency Control in Sendai, Japan, 1745-1748. Korteweg, D. Uber dieFortpflanzungsgeschwindigkeit des Schalles in elastichen Rohren. Ann.Phys. Chem. (1879) 5: 525-37, the contents of which are incorporatedherein.

N−1 displacement 2D maps (also referred to as correlation matrices) arecomputed through the correlation of two consecutive frames i and i+1(1<i<N−1). Each frame is represented by a matrix of pixel values. Thedisplacement maps provide an indication of the local axial movementsbetween frames. Estimation of the axial displacements from the twoconsecutive frames is performed using a speckle tracking algorithm. Inthis algorithm, the time-shifts in the backscattered signals aredetermined between two consecutive frames through cross-correlation ofsmall sliding windows over the entire ultrasound image. For each window,the signal of the frame i and the frame i+1 are cross-correlated. Themaximum of the correlation coefficient gives an estimation of thetime-shift between the two signals. This time-shift can be converted toa spatial displacement by assuming a constant speed of sound for thetissue. This technique can detect displacements on the order of 10 μm.Using small correlation windows of 7.5 mm, the resolution of thedisplacement maps is in the millimeter range. The cross-correlationalgorithm suitable for estimating displacement between consecutive imageframes is described in U.S. Provisional Patent Application No.60/619,247, filed Oct. 15, 2004, which is incorporated by referenceherein. In the exemplary embodiment, a Matlab program Multiframe is usedto compute the displacement maps for the complete sequence of framesobtained at 202, above. Multiframe calls the Matlab routineFunCalculDispl to compute the displacements for the sequence of frames.FunCalculDispl in turn calls the routine Correlation2D.cpp which is a Cprogram that computes the displacement map between consecutive frames.As discussed above, Correlation2D.cpp uses small sliding windows to findthe displacement which maximizes the correlation coefficient for eachpart of the image. In accordance with other embodiments of the presentdisclosure, auto-correlation calculations or coherence calculations, asare known in the art, can be performed.

Two optional threshold procedures can be executed in the procedure 200.At 208, a threshold can be applied on the energy of the signal, in orderto remove the noise that is below a predetermined signal-to-noise ratio.Low energy ultrasound signals (e.g., noise in the cavity of the heart)can be removed from the displacement map according to this method. At210, a threshold can be applied on the correlation coefficient to removeerroneous estimates in the displacements. In the exemplary embodiment,the noise threshold and correlation-coefficient threshold can beimplemented within the routine Correlation2D.cpp. The levels of thethresholds are determined experimentally and can be stored in an inputdata file 110 for processing on the CPU 108. Procedures 206, 208 and 210are illustrated sequentially; however, it is understood that they canoccur simultaneously or any other order to appropriately process thedata. Moreover, one or more of these procedures can be omitted from theprocess described herein.

A video of the sequence of N−1 displacement maps can be assembled tocreate a video of the displacements of the body structure or tissue(212). In the exemplary embodiment, a video of the myocardiumdisplacements is created by this technique.

The video of the displacement map of the myocardium will depict thepropagation of the electromechanical wave. Next, an observation andtracking of the wave propagation (214). Although such tracking can bedone manually, it can be difficult to discern the wave by visualobservation and thus make accurate measurements. Accordingly, wavetracking can be performed by an algorithm, such as TrackPositionWave, aMatlab program which locates the position of the wave front byperforming a zero-crossing calculation on consecutive displacement maps.

The parameters of the electromechanical wave, e.g., velocity, amplitude,attenuation, frequency, etc., can be analyzed at 216. For example, thevelocity of the electromechanical wave can be computed as a function ofits position in the myocardium. As illustrated in FIG. 3, the wall ofthe myocardium is approximated as circular with a radius R, and theorigin of the spherical coordinate system was chosen at the center ofthe cavity. The wavefront of the electromechanical wave was then trackedby its angular coordinate θ. The Matlab function Overlay can be used tocompute the transformation of the raw image into polar coordinates. Thisroutine can also display the displacement map superimposed on theultrasound grayscale data. As an example, the speed of theelectromechanical wave is shown on the FIG. 4 as a function of theangular position.

The ultrasound imaging method described herein has the advantage ofbeing completely non-invasive. In an exemplary embodiment, the systemdescribed herein can be implemented in real-time on commercial scanners.It has been shown that the electrical conductivity is transverselyisotropic with respect to fiber direction, with a longitudinal velocityof about 0.6 m/s and a transverse velocity of about 0.2 m/s (Roth, B. J.(2000), Influence of a perfusing bath on the foot of the cardiac actionpotential. Circulation Research 86, E19-E22; Spach, M. S., Heidlage, J.F., Dolber, P. C., and Barr, R. C. (1998), Extracellular discontinuitiesin cardiac muscle—Evidence for capillary effects on the action potentialfoot. Circulation Research 83, 1144-1164). The electromechanical wavevelocity noted herein was very close to the longitudinal velocity of themechanical wave. The transverse velocity can be measured by usingultrasound imaging and displacement estimation using a 3D imaging probeor a rotational 2D imaging probe. FIG. 5 illustrates a transducer setupfor 2D imaging of the longitudinal waves, and FIG. 6 illustrates atransducer setup for 2D imaging of transverse waves.

The mechanical component of the electromechanical wave is related to theviscoelastic properties of the soft tissue. The elastic properties ofthe myocardium have been widely investigated. The stiffness of themyocardium has been shown to increase during ischemia and recovers afterreperfusion. Thus, early detection of cardiovascular diseases such asischemia and infarction can be strongly improved through non-invasivecharacterization of the local myocardial elasticity.

Low frequency shear (mechanical) waves propagate in soft tissue at lowvelocity (0.5 to 50 m/s). For an isotropic and infinite medium, it hasbeen shown that the velocity of the shear wave is related to the shearmodulus p and the density p by:

$\begin{matrix}{V_{S} = \sqrt{\frac{\mu}{\rho}}} & (1)\end{matrix}$

(Bercoff, J., Tanter, M., and Fink, M. (2004), Supersonic shear imaging:A new technique for soft tissue elasticity mapping. IEEE Transactions onUltrasonics Ferroelectrics and Frequency Control 51, 396-409; Sarvazyan,A. P., O. V. Rudenko, S. D. Swanson, J. B. Fowlkes and S. Y. Emelianov,Shear wave elasticity imaging: A new ultrasonic technology of medicaldiagnostics. Ultrasound Med Biol (1998) 24(9): 1419-1435.) According toanother exemplary embodiment of the disclosed subject matter, a systemcan be implemented to provide early detection of ischemia through themeasure of the velocity of the mechanical wave.

However, the myocardium has also anisotropic mechanical properties andcan be considered as a transverse isotropic medium. As a consequence,two shear waves of different velocities can propagate in the myocardium.Fast mechanical (shear) waves propagate in the direction of the fibers,and slow mechanical (shear) waves propagate in the directionperpendicular to the fibers. The measure of the two wave velocities canbe achieved by using 3D Ultrasound imaging systems or multipleacquisitions of 2D images with a rotation of the transducer (see FIGS.5-6). The wave velocities are related to two elastic constants, μ_(//)the shear modulus in direction of the fibers and μ_(⊥) the cross-fibershear modulus.

$\begin{matrix}{V_{//} = \sqrt{\frac{\mu_{//}}{\rho}}} & (2) \\{V_{\bot} = \sqrt{\frac{\mu_{\bot}}{\rho}}} & (3)\end{matrix}$

The systems and methods described herein can potentially have differentapplications in the field of early detection of cardiovascular diseasesand cardiac imaging.

For example, the measure of the electrical excitation propagation is ofhigh interest in cardiology for early detection of heart diseases butalso for pacing the heart when heartbeat is too slow or irregular. Thepurpose of an artificial pacemaker is to stimulate the heart when eitherthe heart's natural pacemaker is not fast enough or if there are blocksin the electrical conduction system preventing the propagation ofelectrical impulses. Thus, in order to implant the artificial pacemakerat the correct location, the electrical propagation must be determinedaccurately. In vivo imaging of the electrical propagation in the heartcan require implanting an electrode matrix (up to 500 electrodes) tomeasure extracellular potentials at the surface of the heart. Thisinvasive and potentially precarious surgical procedure cannot beperformed on human patients for diagnostic purposes. The presentdisclosure provides a means for determining electrical propagation inthe myocardium of a subject, in the context of achieving an effectiveposition of a pacemaker in the subject. Other methods known in the artinvolve optically-based techniques which also require invasiveprocedures, such as open-chest surgery.

The present disclosure can be further used to create images and therebydetect myocardial ischemia in a subject either having symptoms (e.g.,chest, arm, or chin pain, nausea, shortness of breath, and/or sweating)or a subject subjectively lacking such symptoms (e.g., “silentischemia”), whereby a finding of increased electromechanical wavevelocity (relative to control values) in a region of the myocardium of asubject is consistent with and supportive of a diagnosis of myocardialischemia in that region. The present disclosure can also be used todiagnose, or assist in surgical intervention in, (i) conductiondisturbances, such as re-entry phenomena, or associated withpharmaceutical agents, such as antidepressants or hyperkalemia, (ii)arrhythmias and dysrhythmias (e.g., surgical treatment of ventriculardysrhythmias, diagnosis of low-amplitude atrial fibrillation); and (iii)tissue abnormalities associated with cardiomyopathies or trauma, etc.

Example A—Imaging of Canine Heart

The procedure described hereinabove was performed in an anesthetizedopen-chested dog. The transducer was placed on the anterior wall of theleft ventricle of the heart, to obtain a short axis view. Approximatelyevery two minutes, a sequence of three cardiac cycles was acquiredduring the experiment, with a frame rate of 56 fps. The 2D displacementmaps were estimated using the cross-correlation method (window size: 5mm, 90% overlap). The axial displacements were processed for thedifferent sequences. On the displacement video, two electromechanicalwaves were clearly detected, propagating in the posterior wall of theleft ventricular, from the septum (left side of the images) to thelateral wall (right side). The propagation of the mechanical wavecorresponds to the electrical activity shown on an associated EKG.

The first electromechanical wave is found at the end-diastolic phase ofthe cardiac cycle (which corresponds to the beginning of thecontraction). FIGS. 5(a) through 9(a) show five consecutive frames ofthe propagation of the wave. The location of the electromechanicalwavefront is indicated by arrow W in each of FIGS. 7(a)-11(a). Thedisplacements maps are overlaid to the grayscale ultrasound images (see,FIGS. 7(b)-11(b)). Blue displacements are in the direction of thetransducer (top of the image), and red displacements are in the oppositedirection. As shown in these images, the contraction of the myocardiumstarts on the left side (septum) and propagates to the right side of theimage. In the figures, the blue region appears on the left side of theimages (behind the wavefront), and the red region appears on the rightside of the image (in front of the wavefront). The maximum displacementsshown are 75 μm (dark blue and dark red), and the wave propagates withina few milliseconds. Therefore it is impossible to visually detect thiselectromechanical wave on the grayscale images. The wave speeds asmeasured using the techniques described above are represented in FIG. 4.The wave velocity was found to be approximately 0.6 m/s in the posteriorwall, which was corroborated by invasive electrophysiologicalmeasurements using a matrix of electrodes. Temporary regional ischemiawas then induced by coronary artery ligation. The velocity of theelectromechanical wave was found to increase up to approximately 1.7 m/sin the ischemic region. Although not entirely understood, this strongincrease is believed to be due to an increase of the shear modulus inthe ischemic region or a change in the conduction velocity, or both. (Asecond electromechanical wave has also been detected at the end-systolephase. However, due to its high propagation speed (related to the highcontraction of the myocardium), the propagation was not caught with asufficiently high frame rate. Some evidences of its propagation aredetected in the human experiments, described herein.)

Example B—Imaging of Human Heart

The procedure 200 described hereinabove was performed on a young healthypatient. The transducer was placed on the patient's thorax in order toimage the heart in the short axis view. A sequence of approximately fourcardiac cycles was acquired at a very high frame rate of 170 fps using aVingmed System Five for RF image acquisition. In order to reach such ahigh frame rate, only a small part of the heart (the left ventricle) wasimaged (80×40 mm). The axial displacements were processed for eachframe. On the displacement video, 2 electromechanical waves were clearlyseen, propagating in the posterior wall of the left ventricular (notshown). FIGS. 12(a)-18(a), which are consecutive displacement mapssuperimposed on the grayscale images (FIGS. 12(b)-18(b)), illustrate thepropagation of the electromechanical wave at the end-systole phase. Thespeed was found to be 0.65 m/s in the posterior wall. The location ofthe electromechanical wavefront is indicated by arrow W in each of FIGS.12(a)-18(a).

Example C—Imaging of Cardiovascular Tissue in Mice Animal Preparation

The procedure described hereinabove was performed on anesthetized mice.The mice were anesthetized with tribromoethanol. The hair was removedusing potassium thioglycolate and the mouse was placed in the supineposition on a heating stage (VisualSonics, Toronto ON, Canada) in orderto keep the body temperature steady. ECG signal was obtained from theextremities. The ultrasound probe was placed on the chest or theabdominal wall using degassed ultrasound gel (Aquasonic 100, ParkerLaboratories Inc., Fairfield N.J., USA) as a coupling medium.

RF Signal Acquisition

An ultrasound scanner specifically developed for imaging small animals(Vevo 770, Visualsonics, Toronto ON, Canada) was used in this exemplaryembodiment. The high frequency ultrasound probe was composed of a singlefocused transducer working at 30 MHz, with a focal depth of 12.7 mm. Thetransducer was mechanically rotated and real-time 2D images could beacquired at a frame rate of up to 60 Hz. The field of view was 12×12 mm,the axial resolution was 50 microns, and the lateral resolution was 100microns.

A digitizer (2 channels, 200 MS/s, 14 bits, CS14200, Gage AppliedTechnologies, Lachine QC, Canada) mounted on a PC computer slot wasconnected to the analog RF-output of the ultrasound scanner. Inaddition, two TTL outputs were used to trigger the digitizer on the 2Dframes. This setup allows the real-time acquisition of more than onethousand 2D RF-data, e.g., images.

In the exemplary embodiment, the ultrasound probe was placed on thechest in the parasternal position to obtain a longitudinal (long-axis)view of the left ventricle of the heart. The probe could also bepositioned over the abdomen to obtain a longitudinal view of theabdominal aorta.

Frame Rate Acquisition

In addition to the real-time scanning mode, a high frame rateacquisition mode (EKV) was provided on the scanner in the exemplaryembodiment in order to allow detailed visualization of the heartcontraction. The equipment can operate as quickly as 8000 frames perminute, although the user can see 1000 frames per minute due to droppedcalls. Using this technique, the ultrasound acquisition of each RF-linewas triggered on the mouse ECG. The transducer was slowly rotated andfor each position of the transducer, ultrasound echo signals wererecorded with a pulse repetition frequency (PRF) of 8000 pulses/s duringseveral cardiac cycles. The ECG was simultaneously recorded and thusallowed for the synchronization of the RF-lines based on the R-wavepeak, a reliable peak of the ECG during the cardiac cycle. The completeacquisition duration was approximately 5 min.

To compute the tissue motion, RF-signals and ECG signals were digitizedduring the EKV acquisition and transferred to the computer in real-time.The data were then processed off-line, RF-lines were synchronized usingthe R-wave peak of the ECG signal, and a complete set of 2D ultrasoundRF-data was reconstructed at 8000 fps for one complete cardiac cycle(approximately 150 ms).

Motion Estimation

The motion of the tissue was estimated off-line using a well-knownclassical speckle tracking algorithm (Bonnefous, O. and P. Pesque. Timedomain formulation of pulse-Doppler ultrasound and blood velocityestimation by cross correlation. Ultrason Imaging (1986) 8(2): 73-85).This technique was based on detecting the small local displacements ofthe tissue that occur between two consecutive frames. With the currentmethod, only axial displacements (in the direction of the transducer)were computed. In this algorithm, the time-shifts in the backscattereredsignals were determined between the two consecutive frames throughcross-correlation of small sliding windows over the entire ultrasoundimage. This technique allowed the detection of very small displacementson the order of 1 μm or less (correlation windows of 150 μm, overlapping90%). Finally, the movie of the axial displacements was processed at aframe rate up to 8000 frame/s for the entire cardiac cycle. It isunderstood the lateral displacement can be obtained using the sametechnique.

Frequency Analysis

The axial displacements were analyzed in the frequency domain as afunction of the time. A sliding Blackman window (100 points, 25 ms) asis known in the art, was moved along the displacement variation at afixed depth, in steps of 2 ms. The windowed signals were zero-padded to8192 points and their FFT was calculated. The frequency content of thedisplacements was evaluated graphically by plotting these spectra as afunction of time. Based on this frequency analysis, the transient andthe slow motions of the tissues were separated using a digital filter.The displacement estimates were temporally filtered using an FIRband-pass filter with cut-frequencies of f₁=50 Hz and f₂=500 Hz, whichallows the removal of the low frequency components but also the highfrequency noise.

Wave Velocity

To analyze the propagation of the mechanical waves, the phase velocityof the vibration was determined for an angular frequency co. The wavewas assumed to propagate with a velocity c in a direction r that wasarbitrarily determined on the image by the direction of the wall, and aset of measurement points was selected on this direction. The wavenumber is k=ω/c, and the phase of the wave is φ(r)=kr along thedirection of propagation. The phase was measured as a function of thepropagation distance r, using the Fourier Transform of the temporaldisplacements at the location r computed at the angular frequency co.Finally, the derivative of the phase of the wave with respect todistance was estimated using a linear regression fit on the set ofmeasurements points, and the velocity of the wave at the frequency f wascalculated:

c(f)=2πf/(∂φ/∂r)  (4)

Modulus Estimation

The theory of elastic wave propagation in soft biological tissue wasconsidered in order to derive the Young's modulus of the tissue.Assuming that the medium is infinite and isotropic, the speed of shearwaves propagation could be derived from general equations of the dynamictheory of elasticity. However, it is understood that the propagation ofelastic waves in the myocardium can optionally take into accountadditional characteristics such as the active properties of the musclefibers, the strong anisotropy of the tissue, and/or the geometry of theventricles.

For the transverse wave on the artery wall, a simple model of thepropagation of a pressure wave in a viscoelastic infinite thin conduitfilled with an incompressible fluid is well described by theMoens-Korteweg equation:

$\begin{matrix}{c = \sqrt{\frac{Eh}{2R\rho}}} & (5)\end{matrix}$

where c is the velocity of the wave, E is the Young's modulus of theconduit wall, h is the wall thickness, p is the density of the fluid andR the radius of the tube. According to this equation, the elasticity ofthe vessel wall can be derived from the measurement of the pulse wavevelocity in the artery.

Results of Example C In Vivo Cardiac Imaging

FIG. 19 shows a B-mode image 1910 of a typical parasternal long-axisview obtained in a normal mouse. Image 1910 shows the main structures ofthe left ventricle: the intraventricular septum 1912, the cavity of theleft ventricle 1914, the papillary muscle inside the cavity 1916 and theposterior wall 1918 which is visible due to strong reflections at theepicardium-lung interface. Also shown in image 1910 is the rightventricle 1920, aortic valve 1922, aorta 1924, mitral valve 1926, andleft atrium 1928. In this embodiment, the duration of the averagecardiac cycle was 138 ms. Axial displacements were estimated for thecomplete set of data. In order to keep the displacements at appropriatemagnitudes for the estimation (on the order of 1 μm and to reduce theamount of data, the number of frames was halved, which also reduced theframe rate to 4000 fps.

FIGS. 20(a) and 20(b) show the color-coded axial displacements overlaidonto the grayscale B-mode image for two different phases of the cardiaccycle. During the systolic phase, the contraction of the myocardium isshown by positive displacements (red region) of the posterior wall 2018and negative displacements of the septum 2012 (blue region) (FIG.20(a)). In the diastolic phase, the directions of the displacements ofthe posterior wall 2018 and the septum 2012 (and the colors associatedwith the direction of movement) are reversed during the relaxation (FIG.20(b)). It should be noted that even if a large part of the myocardiumof the posterior wall is not visible, the motion of the epicardiumundergoes similar motion. The time of acquisition of FIG. 20(a) isindicated at point t of FIG. 20(c). The time of acquisition of FIG.20(b) is indicated at point t of FIG. 20(d).

A temporal analysis of the motion was performed for single RF lines ofthe image. The axial displacement along one central line of the image(indicated by the white, dotted vertical line 2050 on FIG. 20(b)) isshown as a function of time in FIG. 21(a) with the corresponding ECGsignal (FIG. 21(d)). (FIGS. 2(a)-(d) are aligned on a temporal basis.)On this line 2050, the displacements of the septum, the papillary muscleand the posterior wall are shown in a M-mode format over two cardiaccycles. It shows the successive main phases of the cardiac cycle: thecontraction of the myocardium (systole) indicated by arrow 2120initiated at the R-wave peak of the ECG, followed by the relaxationphase (diastole) indicated by arrow 2130. The duration of the activecontraction was approximately 50 ms, and that of the relaxation 35 ms.In addition to this slow and large motion, some rapid transientvariations of a few ms were observed at the beginning and at the end ofthe systolic phase, in the septum and the posterior wall.

In order to separate the electromechanical wave from other mechanicalwaves generated by vibrations resulting from valve functions or bloodflow, high-pass filtering was performed. The frequency content of thetissue displacements resulting from vibrations in the septum (at depthof 12.5 mm) was analyzed as a function of time and is shown in FIG.21(b). During the contraction and the relaxation of the heart, themotion of tissue was found to be in the low frequency range of up to 60Hz. However, during the transient motion at the end of systole, muchlarger frequency components were found that ranged between 50 Hz and 500Hz. The same effect was found for the transient motion at the beginningof systole, but the frequency range was limited between 50 Hz and 250Hz. Thus, it was possible to almost completely separate the transientpart of the displacement by filtering out the low frequency component ofthe motion. After filtering the displacements using a FIR band-passfilter with cut-off frequencies f₁=50 Hz and f₂=500 Hz, the twovibrations were clearly visible and are shown on FIG. 21(c) as regions2150 and 2152. These rapid variations occurred within less than 3 msaround the beginning of systole and end-systole.

End of Systole

In order to analyze spatially the vibration around end-systole, weconsidered the data between 52 ms and 70 ms after the peak of theR-wave. FIGS. 22(a)-(d) show a sequence of axial displacements overlaidonto the grayscale B-mode images every 0.6 ms around end-systole. Thissequence uncovers a strong mechanical wave W propagating in thelongitudinal direction of the ventricle along the myocardium, from thebase (right side of the images) to the apex (left side). In other words,as the tissue locally vibrates along the axial direction of the beam(i.e., along the beam axis), a transverse wave propagates along thelateral direction (i.e., in-plane, perpendicular to the beam axis). Asecond wave W′ is shown in FIGS. 22(e)-(f).

The mechanical wave, i.e., generated by localized vibrations in themuscle (FIG. 21(c)), was visible both in the posterior wall and theseptum. Its amplitude was found to be eight times higher in the septum.Only the mechanical wave propagating in the septum is described herein.A set of 60 samples was selected in the septum along the propagationdirection (lateral direction of the image), and the phase of the wavewas computed at different frequencies. Three frequencies were selectedfor which the displacement amplitude was large enough to detect, e.g.with respect to noise level: (*) 82 Hz (●) 246 Hz (⋄) 410 Hz. The phasevelocity of the wave was computed for these frequencies and a largedispersion was found. The distance of propagation was plotted in FIG. 23as a function of the phase of the wave divided by the angular frequency.The phase velocity was found to be 1.20 m/s at 82 Hz, 3.02 m/s at 246 Hzand 4.21 m/s at 410 Hz.

Beginning of Systole

The same analysis was performed at the beginning of systole. Thefiltered data were processed between 0 ms and 20 ms from the peak of theR-wave. FIGS. 24(a)-(f) show a sequence of axial displacements overlaidto the grayscale B-mode images every 2.8 ms around the beginning ofsystole. A strong vibration was found in the septum, but no wavepropagation was visible in the image plane. Therefore, a mechanical wavecan propagate in the perpendicular direction, but was not being observedwith the equipment described herein.

However, the FIG. 24 shows a wave propagating in the posterior wall (seethe white arrows W). The displacements were initiated at the apex (leftside of the images) and then propagated towards the base (right side).The phase velocity was determined using the method previously describedat the frequency of 80 Hz. The distance of propagation was plotted inFIG. 25 as a function of the phase of the wave divided by the angularfrequency. The phase velocity of the wave was obtained using a linearregression fit and was estimated to be 0.44 m/s.

Imaging Under Different Electrical Pacing Conditions

In order to determine that the origin and direction of the wave W wereelectrically induced and driven, mice were also scanned duringright-atrial pacing (at 90 ms corresponding to a heart cycle at sinusrhythm of 100 ms period; FIGS. 26(a)-(e)) and right-ventricular pacing(also at 90 ms; FIGS. 27(a)-(e)). Pacing was achieved usingcatheterization through the right side of the heart, in which thecatheter carried nine electrodes that could be separately activated forvarying the pacing location. In some of the scans, the catheter C waswithin the imaging field-of-view and allowed for imaging of the pacingwave during ventricular pacing (FIGS. 26(c) and 27(c)).

The most pronounced wave propagating during atrial pacing was thecontraction wave, or wave originating at the isovolumic contractionphase, that propagated along the longitudinal direction of themyocardium initiating radial thickening (or, positive (red)displacement) in its path. At atrial pacing (FIG. 26(a)-(e)), thecontraction wave was very similar to the one during sinus rhythm (FIGS.24(a)-(f)), starting at the apex right at the QRS peak and thenpropagating along the posterior wall (generally from right to left inthe figure.) Right-ventricular pacing (FIGS. 27(a)-(e)) induced areverse direction on the contraction wave that now started from the tipof the catheter (close to the base) with two waves propagating from baseto apex, one along the septum and one along the posterior wall(generally from left to right in the figure) (FIG. 27(a)-(e)). Sincepacing occurred using the same mouse, same sonographic view and withoutaffecting the function of the valves or the blood flow, the reversedirection of the propagation of the wave is concluded to be induced bythe change in the origin of the electrical stimulus; thereby, confirmingthat the wave measured is electrically induced.

In Vivo Vascular Imaging

A longitudinal view of the abdominal aorta of a mouse was imaged usingthe high frame rate technique. Axial displacements were calculated, andthe movie of the motion was processed at 8000 fps for a complete cardiaccycle. During the cardiac cycle, the displacements of the artery wallwere found to be very small except after the beginning of systole.Strong displacements of the wall started 10.3 ms after the R-wave peakof the ECG. FIGS. 28(a)-(f) show a sequence of the axial displacementsin color overlaid onto the grayscale B-mode image. A transverse wave Wstarted propagating on the right side of the images (heart side) andthen propagated towards the left side in less than 3 ms. This transversewave was generated from the sudden pressure change of the blood bolustraveling through the vessel, known as the arterial pulsive wave(Nichols, W. and M. F. O'Rourke (1998). Vascular impedance. InMcDonald's: blood flow in arteries: theoretical, experimental andclinical principles. E. Arnold. London).

The phase velocity of the pulse wave was computed at the frequency of200 Hz. The distance of propagation was plotted in FIG. 29 as a functionof the phase of the wave divided by the angular frequency, the phasevelocity was obtained using a linear regression fit and was found to be3.08 m/s. The radius of the vessel R=0.47 mm and the wall thicknessh=0.12 mm were approximately estimated from the B-mode images, and theblood density was assumed to be 1060 kg/m³ (Cutnell, J. and W. Kenneth(1998). Physics, Fourth Edition. New York). Using these parameters, theYoung's modulus of the aorta wall E=78.8 kPa was derived from theMoens-Korteweg equation (Eq. 5), which is what has been typicallyreported for thoracic aorta moduli in biomechanics literature (Fung, Y.C. (1993). Biomechanics—Mechanical Properties of Living Tissues. NewYork).

Electromechanical Activation of Arrhythmias

According to another aspect of the disclosed subject matter, systems andtechniques are provided for electromechanical activation of arrhythmias,including non-transient electromechanical activation of paroxysmal andperiodic arrhythmias in humans in vivo.

Certain treatments of cardiac arrhythmias, such as radio-frequencyablation, can be utilized in clinical practice but can lack a suitablenoninvasive imaging modality to provide insight into the source or focusof an arrhythmia. Cardiac deformations can be imaged at high temporaland spatial resolution to elucidate electrical activation sequences innormal and paced human subjects non-invasively. In this manner, suchimaging can be used to improve planning and monitoring of ablation-basedarrhythmia treatments.

Aspects of the disclosed subject matter include techniques toquantitatively characterize focal and reentrant arrhythmias. For purposeof illustration and not limitation, and as embodied herein,spatio-temporal maps of a full-view of the atrial and ventricularmechanics can be obtained in a single heartbeat. Such maps canillustrate with suitable detail the electromechanical patterns of atrialflutter, fibrillation, and tachycardia. For example and withoutlimitation, during focal arrhythmias, such as premature ventricularcomplex and focal atrial tachycardia, the electromechanical wave imagingtechniques can be utilized to identify the location of the focal zoneand the subsequent propagation of cardiac activation. For purpose ofillustration and not limitation, exemplary electromechanical waveimaging techniques are described in International Application No.PCT/US13/64377, filed Oct. 10, 2013, which is incorporated by referenceherein in its entirety. Additionally or alternatively, and as embodiedherein, during reentrant arrhythmias, such as atrial flutter andfibrillation, Fourier analysis of the strains can show correlatedmechanical and electrical cycle lengths and propagation patterns.

For purpose of illustration and application of the disclosed subjectmatter, high frame rate ultrasound imaging of the heart can be usednon-invasively and in real time to characterize lesser-known mechanicalaspects of atrial and ventricular arrhythmias. Such techniques can alsobe used to assist treatment planning for intraoperative and longitudinalmonitoring of arrhythmias.

Certain imaging systems, such as software-based systems can allowultra-high frame rates, and thus ultrasound imaging can be used to allowunprecedented temporal resolution. For example, such ultrasound imagingsystems can provide a five-fold improvement in the signal-to-noise ratioof cardiac motion and deformation mapping. For example and withoutlimitation, as embodied herein, frame rates up to 2000-5000 frames/s canbe achieved by using defocussed transmissions, which can be suitable fordepths utilized in transthoracic cardiac applications. According toexemplary embodiments of the disclosed subject matter, ultrasoundimaging techniques described herein can be used to map transient strainsoccurring in response to the electrical activation, (e.g., theelectromechanical wave). For example and without limitation, and asembodied herein, such techniques can be used to map transmuralactivation sequences of normal and abnormal hearts and to locate pacingsites in patients undergoing cardiac resynchronization therapy.

According aspects of the disclosed subject matter, systems andtechniques are provided to analyze and characterize the mechanicalbehavior of the atria. For purpose of illustration and not limitation,and as embodied herein, systems and techniques disclosed herein can beutilized to analyze and characterize the atria during certain types ofcardiac arrhythmia, including and not limitation to, prematureventricular complex, focal tachycardia, atrial flutter, and atrialfibrillation. While Electromechanical Wave Imaging (EWI) can be suitableto characterize focal rhythms such as premature ventricular complex andfocal tachycardia, EWI can have difficulty describing and/orcharacterizing reentrant rhythms such as atrial flutter andfibrillation. Accordingly, systems and techniques described herein areprovided to characterize electromechanical strains, including andwithout limitation, during reentrant rhythms based on Fourier analysis.Exemplary embodiments of the disclosed subject matter can include asingle acquisition sequence of electromechanical activation mapping thatcan be used for standard EWI and/or for Fourier analysis ofelectromechanical strains. Electromechanical activation mapping cancharacterize electromechanical strain propagation patterns during bothfocal and reentrant arrhythmias. In this manner, systems and techniquesdescribed herein can determine that local deformations of the atria canbe closely correlated with their electrical activation. As such, systemsand techniques described herein can be used to determine characteristicsof cardiac mechanics in arrhythmia, to plan ablation treatments, and tomonitor the efficacy of such treatments non-invasively, longitudinallyand in real-time.

Example D—Imaging Electromechanical Activity During Arrhythmia

For purpose of illustration and confirmation of the disclosed subjectmatter, exemplary techniques for imaging electromechanical activation ofarrhythmias are described. The systems and techniques described hereincan be performed, for purpose of illustration and not limitation, onhuman subjects. The human subjects can undergo a diagnostic ultrasoundscan, and as embodied herein, can occur a few minutes to a few hoursprior to electroanatomic mapping and ablation. The cardiac arrhythmiasof the patients can be confirmed during electroanatomic mapping andablation to be, for example and without limitation, one or more ofpremature ventricular complex (n=1), atrial flutter (n=5), focal atrialtachycardia (n=1), and atrial fibrillation (n=1). Additionally, a normalhuman subject can be imaged as a control for purpose of comparison.

Additionally, and as embodied herein, strain maps can be generated, forexample and without limitation using similar techniques as describedherein for single-heartbeat electromechanical wave imaging (EWI). Forexample and without limitation, as embodied herein, a Verasonics systemwith a 2.5-MHz probe can be calibrated and customized to adhere to FDAstandards, including measurements of mechanical index and of peakspatio-temporal-average intensity. The Verasonics system can becalibrated to have an acoustic power output that is similar toconventional clinical scanners. Such calibration can be performed bymeasuring the peak pressure and/or intensity (e.g., spatial-peaktemporal average intensity, also referred to as Ispta) of the Verasonicssystem to ensure that its mechanical index (MI) is within FDAguidelines. The ultrasound scan can include two sequences. As embodiedherein, in a motion-estimation sequence, a circular ultrasonic wave canbe emitted with a virtual focus of 10.2 mm behind the probe at 2000 fpsduring 2 seconds. Additionally or alternatively, as embodied herein, astandard B-mode acquisition can be performed during 1.5 seconds todepict the heart anatomy. Frames from the motion-estimation sequence canbe reconstructed by generating a plurality of beams, for example and asembodied herein 128 beams, in post-processing using a delay-and-sumalgorithm with a reconstructed sampling frequency of 20 MHz. As embodiedherein, the motion-estimation rate and the motion-sampling rate can beset to 1000 and 2000 fps, respectively. The window for motion-estimationcan be 9.2 mm with an overlap of 95.8% (window shift of 0.3 mm), and thekernel strain estimation can be set to 4.9 mm. For purpose ofillustration and not limitation, and as embodied herein, the techniquesdescribed herein for beamforming, motion-estimation, strain estimation,spatial moving-average of the strains (12 mm by 10 lines), and theautomated contour tracking technique can be performed off-line on agraphics processing circuit (embodied herein as a Tesla graphicsprocessing unit) and a Matlab parallel processing toolbox at a computingspeed of 2.4 frames/s.

Furthermore, and as embodied herein, focal and reentrant arrhythmias canbe analyzed differently for patients with different types of rhythms.For purpose of illustration and not limitation, FIG. 30A illustratesstrains mapped in subjects having sinus rhythm. FIG. 30B illustratesstrains mapped in subjects having atrial flutter. FIG. 30C illustratesstrains mapped in subjects having atrial fibrillation.

As illustrated for example in FIG. 30A, for subjects with sinus rhythm,the strains in one location, (e.g., one pixel in the left atrium) canpresent two representative events over time that correspondapproximately to the beginning and the end of systole: end-systole, andend-diastole. By tracking the onset (e.g., the first zero-crossing) ofthese representative events for each pixel of the heart walls,isochrones maps can be generated. Isochrones correlated to electricalisochrones can be obtained, for example and without limitation, bytracking the propagation front of the end-diastole electromechanicalactivation. As illustrated for example in FIG. 30B, for atrial flutterpatients, a similar location in the left atrium (LA) illustrates thatstrains can be periodic, which, in some cases, can be represented by asingle frequency. Alternatively, as illustrated for example in FIG. 30C,a plurality of frequencies can be observed in a patient with atrialfibrillation, and as such, analysis based on the Fourier transform mightcan be utilized. During atrial fibrillation, the strains can be chaoticand no period of zero strains, similar to the one in FIG. 30A, can beobserved.

In addition, and as embodied herein, the onset of contraction can bedetermined, for example in subjects who have focal rhythms such as sinusrhythm and focal tachycardia, as the first zero-crossing of theincremental strains occurring after the onset of the P-wave on theelectrocardiogram (ECG), which can utilize the EWI techniques describedherein. Additionally or alternatively, as embodied herein, in atria withreentrant arrhythmia, during flutter and fibrillation, a high-resolutionFourier transform can be performed using a generalized Goertzelalgorithm for interpolation in Fourier space on 1.5-second longincremental strains signals for each individual pixel in the atria. Forpurpose of illustration and comparison with conventional ECGmeasurements, and without limitation, frequencies can be converted tocycle lengths, hereinafter referred to as mechanical cycle length (MCL).As embodied herein, peak MCL maps can be generated by selecting the MCLwith the highest amplitude within the physiologically-relevant 100-330ms range for each pixel. Additionally or alternatively, and as embodiedherein, peak cycle lengths histograms can be constructed and compared tothe electrical cycle length measured directly during the electroanatomicmapping and ablation.

Focal Rhythms

FIG. 31 illustrates an EWI cine-loop and isochrones during focalrhythms. FIG. 31A illustrates the atria of a normal subject, withpropagation from the right atrium (RA) to the LA. The electromechanicalactivation regions 3110 can originate in the right atrium and propagatetowards the left atrium as illustrated in the exemplary EWI cine-loop inFIG. 31A.

FIG. 31B illustrates an EWI cine-loop depicting the atria of a subjectundergoing a focal atrial tachycardia, which can have a focus locatedhigh in the left atrium (LA). With reference to FIG. 31B, as embodiedherein, electrical mapping of this patient has not been completed in theLA. The EWI in FIG. 31B illustrates electromechanical activation 3120originating high in the LA and propagating into both atria, and furtheractivation can be detected in the ventricles.

FIGS. 31C and 31D each illustrate isochrones obtained from a patientwith ventricular tachycardia. FIG. 31C illustrates an isochrone of theventricular tachycardia patient during sinus rhythm. FIG. 31Dillustrates an isochrone of the ventricular tachycardia patient duringpremature ventricular complex. EWI was performed during sinus rhythm andduring pre-ventricular contraction. The EWI isochrones obtained duringsinus rhythm, as shown for example in FIG. 31C, depict propagation fromthe RA, into the LA and into the ventricles, as previously shown forpurpose of illustration and comparison in normal patients. When thispatient underwent premature ventricular complex, as illustrated forexample in FIG. 31D, the region that was activated early in theventricle during sinus rhythm (e.g., from the ventricles to the atria)triggered the entire electromechanical activation sequence. Duringpremature ventricular complex, electromechanical activation canoriginate from the lateral wall, and can propagate toward the atria andinto the atria. Early activation of the septum can indicate a potentialrecruitment of the Purkinje network.

Reentrant Rhythms

FIG. 32 illustrates the electromechanical behavior of a heart undergoingatrial flutter, including the analysis of reentrant arrhythmias using asingle frequency flutter case. FIG. 32A illustrates an exemplary peakMCL map, and as depicted, a single MCL is representative. The peak cyclelength map of FIG. 32A indicates, for each pixel of the atria, whichcycle length is representative in the Fourier spectrum. FIG. 32Billustrates a histogram of the cycle length which can be used todetermine, among all the pixels of the atria, which cycle lengthrepresents atrial contraction. With reference to FIG. 32B, as embodiedherein, one peak cycle length of 294 ms can be identified. FIG. 32Cillustrates a phase map analyzing the phase of the MCL of FIG. 32B inFourier space. As shown for example in FIG. 32C, as embodied herein, apropagation pattern originates from the right atrium (RA) near thetricuspid valve towards the LA. The phase corresponding to the 294 mscycle length can be retrieved from the Fourier spectrum and used to mapthe propagation of the mechanical oscillation at 294 ms. In this manner,the propagation direction can be determined. With reference to FIG. 32C,as embodied herein, the electromechanical activation propagated from theRA to the LA. FIG. 32D illustrates the corresponding intracardiacelectrograms obtained a few hours after the imaging procedure. Withreference to FIG. 32D, as embodied herein, the electrical cycle lengthwas 283 ms.

Additionally or alternatively, and as embodied herein, atrial fluttercases can exhibit different patterns. Indeed, certain cases presentedwith two dominant frequencies can be separated between the left andright atria, whereas certain electrophysiological data can indicate thatonly one reentrant circuit was present.

FIG. 33A illustrates two examples of such atrial flutter cases. FIG. 33Aillustrates peak MCL maps of two exemplary atrial flutter patients. Asshown for example in FIG. 33A, two representative frequencies can beidentified in each patient, with the shorter cycle length located in theRA. A relationship between the MCL and the electrical cycle length canbe obtained, for example and as embodied herein, by performing thisanalysis in multiple patients, and choosing the peak cycle lengthclosest to the electrical cycle length. For purpose of illustration andconfirmation of the disclosed subject matter, such an analysis of MCLand electrical cycle length was conducted for five exemplary patients.FIG. 33B is a graph illustrating the results of the five exemplarypatients. With reference to FIG. 33B, and as embodied herein, at leastone representative MCL was very close to the electrical cycle length.FIG. 33B illustrates that electromechanical cycle length and/or MCL canbe correlated with the electrical cycle length with a correlation of0.96 and a slope of 1.1.

FIGS. 33C and 33D together illustrate results from one exemplary patientundergoing atrial fibrillation. FIG. 33C illustrates a peak MCL mapdepicting multiple clustered dominant frequencies. For purpose ofillustration and not limitation, the separation into these dominantfrequencies is illustrated by the histogram shown in FIG. 33D. Withreference to FIG. 33D, the peak cycle length map during atrialfibrillation depicts further spatial fragmentation of the peak cyclelength.

Aspects of the present disclosed subject matter illustrateelectromechanical activation mapping to identify the site of cardiacrhythm mechanisms during arrhythmia in humans and to characterize suchcardiac rhythm mechanisms, which can lead to improved treatments andclinical management. Certain clinical practices utilize minimallyinvasive techniques to obtain precise maps of the activation of theatria and ventricles. Such techniques can be costly, time-consuming, andcarry some degree of risk, and hence can be challenging to providecomplete activation maps before and after treatment, as well as duringcatheter procedures.

Aspects of the present disclosed subject matter illustrate methods forelectromechanical activation mapping during reentrant and focalarrhythmias. For purpose of illustration and not limitation, and asembodied herein, exemplary techniques are provided for imagingspatiotemporal mechanics of arrhythmias with high accuracy and spatialand temporal resolutions in a full field of view in humans. Theseexemplary techniques can provide for characterization of anelectromechanical propagation pattern and/or representative mechanicalcycle lengths, which can correspond with their electrophysiologicalequivalents.

For purpose of illustration and not limitation, and as embodied herein,focal rhythms can behave similarly to paced rhythms. For example andwithout limitation, focal rhythms can have a single source ofelectromechanical activation located in the vicinity of the earliestelectrical activation. As embodied herein, EWI can be used tocharacterize the propagation of electromechanical activation, which canpropagate from an atria's sinus node and from the bundle branch andwhich can terminate in the ventricles during ventricular pacing.Electromechanical activation propagation patterns similar to pacing canoccur in a patient during premature ventricular complexes. Theelectromechanical activation sequence of the same patient during sinusrhythm can be similar to that of normal subjects. For example, and asembodied herein, in a patient with atrial tachycardia, theelectromechanical activation propagation pattern can indicate a sourcelocated near the roof of the LA, in accordance with electrical mapping.As such, an exemplary application of non-invasive, ultrasound-based,electromechanical activation mapping is provided, which can be performedduring or prior to invasive procedures. For purpose of illustration andnot limitation, prior knowledge of an electromechanical source locatedin the LA can allow for clinical preparation. For example, and asembodied herein, such prior knowledge can be used to determine whethertransseptal access would be obtained during treatment and to performrisk-benefit analysis to determine the best course of treatment (e.g.,pharmacological vs. ablation treatment).

Additionally, and as embodied herein, the electromechanical activationmaps can be correlated with their electrical counterpart, at least inpart of the atrial tissue, during atrial flutter. For example, and asembodied herein, a single representative frequency can be identified,and the phase of that frequency can indicate a propagation directionfrom the cavotricuspid isthmus region to the RA and LA, which can occurduring typical atrial flutters. Additionally or alternatively, and asembodied herein, other behaviors can be identified in the atria,including and without limitation, one part of the atria that contractswith the same frequency as the electrical activation and another regionthat does not contract with the same frequency. As such, mapping themechanics of the heart can identify regions of the heart in which themechanical and electrical activities appear to be decoupled. Furtherspatial fragmentation of the periodicity of the mechanics of the atriacan be observed during fibrillation. Such techniques can determinecharacteristics of the atrial mechanics during arrhythmia, including inthe progression from flutter to fibrillation and vice versa.

For purpose of illustration and not limitation, deformation of the atriacaused by the onset of ventricular contraction and relaxation can affectcertain aspects of the techniques described herein. For example, and asembodied herein, such a deformation can affect frequency analyses basedon multiple activation cycles, which can be due at least in part to therelatively short acquisition time of these processes. Filtering and thedevelopment of longer acquisition sequences can inhibit or prevent suchatrial deformation.

Certain non-invasive electrical mapping techniques can be utilized toexamine the epicardium, and can assume an immobilized heart function. Amechanical assessment of the atria can be utilized, for example, byelectrophysiologists or interventional cardiologists to achieve theadvantages described herein. According to certain clinical practices,echocardiograms can be performed on arrhythmia patients. Othernon-invasive electrical mapping techniques can utilize on time-consumingand costly high resolution CT or MRI scans. The electromechanicalactivation mapping systems and techniques described herein can beobtained separately from, or in conjunction with, echocardiograms.

As embodied herein, mapping the electromechanical activity duringarrhythmias non-invasively with real-time feedback can be used determinecharacteristics of atrial mechanics in the evolution and perpetuation ofarrhythmias. Furthermore, and as embodied herein, such a mapping can beused to predict the origin site of arrhythmias and the mechanism andmonitoring of intervention outcomes.

It will be understood that the foregoing is only illustrative of theprinciples of the present disclosure, and that various modifications canbe made by those skilled in the art without departing from the scope andspirit of the present disclosure.

What is claimed is:
 1. A method for mapping electromechanical activityduring an arrhythmia, comprising: obtaining image information of a heartof a subject using an imaging device; generating a strain map of theheart from the image information; determining from the strain mapoccurrences of a first electromechanical event of the heart and a secondelectromechanical event; generating a spatio-temporal map of atrial andventricular mechanics of the heart by tracking the onset of the firstand second event for each pixel of a heart wall of the subjectidentified from the image information; and identifying, using thespatio-temporal map, a representative mechanical cycle associated with acontraction of the heart; and determining a type of cardiac arrhythmiapresent in the heart from the information collected in the ultrasoundscan of the heart.
 2. The method of claim 2, further comprisingdetermining that the cardiac arrhythmia present in the heart comprisesfocal rhythms, wherein generating the spatio-temporal map furthercomprises determining an onset of ventricular contraction by identifyinga first zero-crossing of an incremental strains occurring after an onsetof a P-wave on an electrocardiogram.
 3. A system for mappingelectromechanical activity during an arrhythmia comprising: a processoradapted to: obtain image information of a heart of a subject using animaging device; generate a strain map of the heart from the imageinformation; determine, from the strain map occurrences of a firstelectromechanical event of the heart and a second electromechanicalevent; generate a spatio-temporal map of atrial and ventricularmechanics of the heart by tracking the onset of the first and secondevent for each pixel of a heart wall of the subject; and identify, usingthe spatio-temporal map, a representative mechanical cycle associatedwith a contraction of the heart; wherein the processor is furtherconfigured to determine a type of cardiac arrhythmia present in theheart from the information collected in the ultrasound scan of theheart.
 4. The system of claim 3, wherein the processor determines thatthe cardiac arrhythmia present in the heart comprises focal rhythms, andwherein the processor generates the spatio-temporal map by determiningan onset of ventricular contraction by identifying a first zero-crossingof an incremental strains occurring after an onset of a P-wave on anelectrocardiogram.